Black Hole Production Limits

Semiclassical Black Holes

INSPIRE  
VALUE (GeV) DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
1
SIRUNYAN
2018DA
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ multijet
2
AAD
2016N
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ multijet
3
AAD
2016O
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \ell}}{+}$ ( ${{\mathit \ell}}{{\mathit \ell}}$ $/$ ${{\mathit \ell}}{{\mathit j}}$ $/$ ${{\mathit j}}{{\mathit j}}$)
4
AAD
2013AW
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \mu}}{{\mathit \mu}}$
1  SIRUNYAN 2018DA use 35.9 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for semiclassical black holes decaying to multijet final states. No excess of events above the expected level of standard model background was observed. Exclusions at 95$\%$ CL are set on the mass threshold for black hole production as a function of the higher-dimensional Planck scale for rotating and nonrotating black holes under several model assumptions (ADD, 2, 4, 6 extra dimensions model) in the $7.1 - 10.3$ TeV range. These limits supersede those in SIRUNYAN 2017CP.
2  AAD 2016N use 3.6 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for semiclassical black hole decays to multijet final states. No excess of events above the expected level of Standard Model background was observed. Exclusion contours at 95$\%$ C.L. are set on the mass threshold for black hole production versus higher-dimensional Planck scale for rotating black holes (ADD, 6 extra dimensions model).
3  AAD 2016O use 3.2 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for semiclassical black hole decays to high-mass final states with leptons and jets. No excess of events above the expected level of Standard Model background was observed. Exclusion contours at 95$\%$ C.L. are set on the mass threshold for black hole production versus higher-dimensional Planck scale for rotating black holes (ADD, 2 to 6 extra dimensions).
4  AAD 2013AW use 20.3 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for semiclassical black hole decays to like-sign dimuon final states using large track multiplicity. No excess of events above the expected level of Standard Model background was observed. Exclusion contours at 95$\%$ C.L. are set on the mass threshold for black hole production versus higher-dimensional Planck scale in various extra dimensions, rotating and non-rotating models.
References:
SIRUNYAN 2018DA
JHEP 1811 042 Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
AAD 2016N
JHEP 1603 026 Search for Strong Gravity in Multijet Final States Produced in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV using the ATLAS Detector at the LHC
AAD 2016O
PL B760 520 Search for TeV-Scale Gravity Signatures in High-Mass Final States with Leptons and Jets with the ATLAS Detector at $\sqrt {s }$ = 13 TeV
AAD 2013AW
PR D88 072001 Search for Microscopic Black Holes in a Like-Sign Dimuon final State using Large Track Multiplicity with the ATLAS Detector